17.50.+h Quantum Hall systems

Topological insulators in dynamically generated lattices

Date: 
2013-04-24 - 2013-12-06
Author(s): 

O. Dutta, A. Przysiezna, M. Lewenstein

Reference: 

arXiv:1301.4156 [cond-mat.quant-gas]

Topological insulators are of fundamental and technological importance due to their exotic excitations that allow for robust transport of charges (matter) on the boundary and thus have potential applications in spintronics, quantum computing and spintomics.

Quantum Hall phases of two-component bosons

Date: 
2013-10-14 - 2013-12-05
Author(s): 

Tobias Graß, David Raventós, Maciej Lewenstein, Bruno Juliá-Díaz

Reference: 

arXiv:1310.3709 [cond-mat.quant-gas]

The recent production of synthetic magnetic fields acting on electroneutral particles, like atoms or photons, has boosted the interest in the quantum Hall physics of bosons. Adding pseudospin-1/2 to the bosons greatly enriches the scenario, as it allows them to form an interacting integer quantum Hall (IQH) phase with no fermionic counterpart.

Topological phases in small quantum Hall samples

Date: 
2013-10-07 - 2013-12-05
Author(s): 

Tobias Graß, Bruno Juliá-Díaz, Maciej Lewenstein

Reference: 

arXiv:1310.1817 [cond-mat.quant-gas]

Topological order has proven a useful concept to describe quantum phase transitions which are not captured by the Ginzburg-Landau type of symmetry-breaking order. However, lacking a local order parameter, topological order is hard to detect.

Interactions in Electronic Mach-Zehnder Interferometers with Copropagating Edge Channels

Date: 
2013-07-17
Author(s): 

Luca Chirolli, Fabio Taddei, Rosario Fazio, Vittorio Giovannetti

Reference: 

Phys. Rev. Lett. 111, 036801 (2013)

Fractional quantum Hall states in lattices: Local models and physical implementation

Date: 
2013-04-23
Author(s): 

Anne E. B. Nielsen, German Sierra, J. Ignacio Cirac

Reference: 

arXiv:1304.0717v2

The fractional quantum Hall (FQH) effect is one of the most striking phenomena in condensed matter physics. It is described by a simple Laughlin wavefunction and has been thoroughly studied both theoretically and experimentally. In lattice systems, however, such an effect has not been observed, there are few simple models displaying it, and only few mechanisms leading to it are known.

From Rotating Atomic Rings to Quantum Hall States

Date: 
2011-07-22
Author(s): 

M. Roncaglia, M. Rizzi, and J. Dalibard

Reference: 

Sci. Rep. 1, 43 (2011)
doi:10.1038/srep00043

Considerable efforts are currently devoted to the preparation of ultracold neutral atoms in the strongly correlated quantum Hall regime. However, the necessary angular momentum is very large and in experiments with rotating traps this means spinning frequencies extremely near to the deconfinement limit; consequently, the required control on parameters turns out to be too stringent. Here we propose instead to follow a dynamic path starting from the gas initially confined in a rotating ring.

Controlled coupling of spin-resolved quantum Hall edge states

Date: 
2011-11-30
Author(s): 

B. Karmakar, D. Venturelli, L. Chirolli, F. Taddei, V. Giovannetti, R. Fazio, S. Roddaro, G. Biasiol, L. Sorba, V. Pellegrini, F. Beltram

Reference: 

Phys. Rev. Lett. 107, 236804 (2011)

Topologically-protected edge states are dissipationless conducting surface states immune to impurity scattering and geometrical defects that occur in electronic systems characterized by a bulk insulating gap. One example can be found in a two-dimensional electron gas (2DEG) under high magnetic field in the quantum Hall regime. Based on the coherent control of the coupling between these protected states, several theoretical proposals for the implementation of information processing architectures were proposed.

From Rotating Atomic Rings to Quantum Hall States

Date: 
2011-07-25
Author(s): 

M. Roncaglia, M. Rizzi, J. Dalibard

Reference: 

M. Roncaglia, M. Rizzi & J. Dalibard
From rotating atomic rings to quantum Hall states
Scientific Reports 1, 43 (2011)

Considerable efforts are currently devoted to the preparation of ultracold neutral atoms in the strongly correlated quantum Hall regime. However, the necessary angular momentum is very large and in experiments with rotating traps this means spinning frequencies extremely near to the deconfinement limit; consequently, the required control on parameters turns out to be too stringent. Here we propose instead to follow a dynamic path starting from the gas initially confined in a rotating ring.

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